[PDF] [PDF] QFT II Solution 7 - UZH - Physik-Institut

Starting from the full QCD-Lagrangian with gauge-fixing and Fadeev-Popov term, LQCD = - 1 4 Fa µνFa sponding Feynman rules using path-integral methods Solution The kinetic term for the ghost field leads to the propagator G gh ab



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[PDF] QFT II Solution 7 - UZH - Physik-Institut

Starting from the full QCD-Lagrangian with gauge-fixing and Fadeev-Popov term, LQCD = - 1 4 Fa µνFa sponding Feynman rules using path-integral methods Solution The kinetic term for the ghost field leads to the propagator G gh ab



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